A Model of the Bat's Vertical Sweetness Gradient
Total Page：16
File Type：pdf, Size：1020Kb
A Model of the Bat’s Vertical Sweetness Gradient David G. Baldwin HylaPark, Inc., 6548 Via Barona, Carlsbad, CA, USA 92009 A. Terry Bahill Systems and Industrial Engineering Dept., University of Arizona, Tucson, AZ, USA 85721-0020 ABSTRACT: Sweetness is defined as the probability of attaining a base hit. The sweetness of a specific bat/ball collision is found by determining the ball's vertical launch characteristics, the range and hang time or ground time of the batted ball and, finally, the probability of batter success. An example is presented to demonstrate feasibility and how the model might be used. INTRODUCTION Warren Spahn summed up his pitching strategy with a pithy aphorism - “Hitting is timing. Pitching is upsetting timing.” The great coach Johnny Sain advised his pitchers to avoid showing batters consecutive pitches of the same speed. The most difficult part of the batter’s task is judging the speed of the pitch and this must be done early in its flight (Adair, 2002; Bahill and Baldwin, 2004). Once the batter begins the swing, the bat’s momentum precludes alteration of the timing or height of the swing. The batter must determine pitch speed in order to estimate the ball's height at impact because the ball is in a free fall throughout its flight. Misjudgment of the ball’s speed results in a vertical error in the swing (e.g., underestimation of pitch speed results in anticipation that the potential contact point will be lower than its actual location). The vertical offset between the trajectory line of the ball’s center and the trajectory line of the transverse center of the bat is a major factor determining the vertical launch characteristics of the ball immediately after collision with the bat. How is this offset related to the batter’s probability of success? We describe a bat/ball collision model relating offset and several other collision parameters to the behavior of the batted ball, which, in turn, is associated with a success probability function for the batter. Batter success is defined as the attainment of a base hit and sweetness (a bat property) is the probability of success for a given bat/ball collision. DESCRIPTION OF THE MODEL Baseball and softball batters swing a narrow cylinder with the axis more or less parallel with the ground. Thus, the transverse curvature of the bat’s face (hitting surface) is a vertical curvature. In combination with the vertical offset of the bat and ball trajectories, this vertical curvature strongly influences the ball’s vertical launch velocity, angle, and spin rate. These launch characteristics can be included in a vector describing a specific point on the bat’s face; a vector field can specify the launch characteristics of all the points on the face. Each vector determines the batted ball’s behavior – the distance it travels in the air until it first strikes the ground (range), how long it stays in the air (hang time), and, for ground balls, the time taken for the ball to reach the positional arc of infielders (ground time). The set of success probabilities associated with a specific vertical arc on the bat’s face is called the vertical sweetness gradient of that arc. The face’s vector field represents sweetness gradients in both the longitudinal (horizontal) and transverse (vertical) dimensions of the bat. However, we restrict our current discussion to vertical collision considerations and the radial placement of the ball in play in fair territory. Figure 1 illustrates the initial vertical configuration of the bat and ball at the instant of collision. The initial parameters of the collision are: (1) Initial velocity vector of bat’s contact point (vbat, 0). (2) Initial normal component of the bat’s velocity vector (vbat, 0, n). (3) Initial tangential component of the bat’s velocity vector (vbat, 0, t). (4) Initial velocity vector of ball (vball, 0). (5) Initial normal component of the ball’s velocity vector (vball, 0, n). (6) Initial tangential component of the ball’s velocity vector (vball, 0, t). (7) Offset distance (D) from the ball’s center perpendicular to the trajectory plane of the bat's transverse center (8) Vertical angle (θ) between the line connecting ball and bat centers (line of centers) and the horizontal plane (z = 0). (9) Vertical angle (γ) between the horizontal plane and the ball’s trajectory plane.. (10) Vertical angle (ψ) between the horizontal plane and the bat’s trajectory plane. (11) Mass of bat (mbat). (12) Mass of ball (mball). (13) Radius of bat at contact point (rbat). (14) Radius of ball (rball). (15) Coefficient of restitution (CoR) of the bat/ball impact. (16) Coefficient of friction (µ) of the bat/ball impact. (17) Angular velocity (ωball, 0) of the pitch. The characteristics mball, rball, CoR, and µ will be considered constants. The values of CoR and µ must be derived empirically. The resultant vectors and angles used to calculate launch velocity and angle are: (1) Resultant velocity vector of bat’s contact point (vbat, R). (2) Resultant normal component of the bat’s velocity vector (vbat, R , n). (3) Resultant tangential component of the bat’s velocity vector (vbat, R , t). (4) Resultant velocity vector of ball (vball, R). This is called the “launch velocity”. (5) Resultant normal component of the ball’s velocity vector (vball, R, n). (6) Resultant tangential component of the ball’s velocity vector (vball, R, t). (7) Vertical angle (φ) between the line of centers and vball, R. (8) Vertical angle (λ) between the horizontal plane (z = 0) and vball, R. This is called the “launch angle”. We also calculate the vertical launch spin rate (ωball, R) and specify air density (ρ). Fig. 1. Initial vertical configuration of the bat/ball collision. The model is set in the x-z plane of a coordinate system with origin at the contact point, three feet in front of the vertex of home plate and at a height of three feet. The positive z axis points upward, positive x axis points toward the pitcher, and positive y axis points out of the plane (Sawicki, Hubbard, and Stronge, 2003). In Fig. 1, the x-z plane is reoriented so the x′ axis lies along the bat/ball line of centers and the z′ axis is tangential to the ball/bat contact point. Angular velocity is positive for pitch topspin and for batted ball backspin. D is positive if the bat undercuts the ball. The angle of descent (γ) of an average fastball is about ten degrees (Adair, 2002; Watts and Bahill, 2000) and batters generally uppercut the ball (ψ) at ten degrees or more. BALL’S LAUNCH VELOCITY, ANGLE, AND SPIN RATE The ball’s launch parameters are calculated by decomposing the initial velocities of the bat and ball into their normal and tangential components at the point of contact. These velocities are used with the principles of conservation of momentum and conservation of energy to yield resultant normal and tangential velocities for the ball, which are then used to calculate the launch velocity of the ball and the angles φ and λ. The batted ball angular velocity is calculated from the normal and tangential linear velocities of the ball and bat and the ball’s initial angular velocity. The collision of two partially elastic bodies with friction is described by numerous authors (e.g., Goldsmith, 1960). The first step in building the model is to calculate θ and, from this, the normal and tangential components of the initial velocity vectors. -1 The vertical angle of the line of centers, θ = ψ + sin (D / (rbat + rball)). The initial velocity components of the ball are vball, 0, n = vball, 0 cos θ and vball, 0, t = vball, 0 sin θ. The initial velocity components of the bat are vbat, 0, n = vbat, 0 cos θ and vbat, 0, t = vbat, 0 sin θ. The resultant normal velocity of the ball (Bahill and Watts, 2000) is vball, R, n = vball, 0, n – (1 + CoR) [( mbat vball, 0, n - mbat vbat, 0, n / (mball + mbat) ] Calculation of relative tangential velocity, resultant angular velocity of the ball, and final launch angle, λ, is described by Sawicki, et al. (2003) and by Watts and Baroni (1989). In these models, friction acts in the direction opposite to the slip of the ball. If friction is large enough, it halts the relative tangential velocity (the combined velocities of bat and ball surfaces relative to the contact point). When this occurs, slippage ceases, the ball sticks to the bat, and the ball begins to roll, contributing to the launch angular velocity. These models account for bat recoil and assume conservation of linear and angular momentum for tangential ball and bat motions. Both models ignore deformation of the ball during collision (they assume it remains a perfect sphere). RANGE, HANG TIME, AND GROUND TIME The launch velocity, angle, and spin rate are the input data into equations (Watts and Bahill, 2000) to calculate the batted ball’s range and hang time. The vertical distance 2 traveled by the batted ball (without regard to lift or drag) is z = vz0 t - 0.5 gt , where vz0 is the vertical velocity of the ball, t is the hang time, and g is the acceleration rate of gravity at the surface of the earth (32.17 ft/sec2). The horizontal distance traveled (again ignoring lift and drag) is x = vx0 t, where vx0 is the horizontal velocity component. The vertical rotation of the ball creates a Magnus force acting vertically perpendicular to the trajectory. This force tends to lift the ball (if backspin) or depress 3 the ball (if topspin).